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FPTE-1.2.1


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توضیحات

The FPTE package is a collection of tools for finite pressure temperature elastic constants calculation. Features include, but are not limited to stress-strain method for getting second order elastic tensors using DFT package VASP as well as, ab initio molecular dynamic method for temperaturedependent elastic constants.
ویژگی مقدار
سیستم عامل -
نام فایل FPTE-1.2.1
نام FPTE
نسخه کتابخانه 1.2.1
نگهدارنده []
ایمیل نگهدارنده []
نویسنده Mahdi Davari
ایمیل نویسنده Mahdi.Davari@iCloud.com
آدرس صفحه اصلی https://github.com/MahdiDavari/FPTE
آدرس اینترنتی https://pypi.org/project/FPTE/
مجوز -
# Finite Pressure Temperature Elasticity (FPTE) package <a href="https://ibb.co/gJpS7Js"><img src="https://i.ibb.co/VTZgNTX/Stress-Strain.jpg" alt="Stress-Strain" border="0" /></a> ## Installation ### Dependencies FPTE requires: - Python (>= 3.7) - NumPy (>= 1.16.5) - Pandas (>= 0.25.3) - Matplotlib (>= 2.2.4) - joblib (>= 0.11) FPTE 1.2.0 and later require Python 3.7 or newer. FPTE 1.1.0 and later require Python 3.4 or newer. FPTE plotting capabilities (i.e., functions start with `plot_` and classes end with "Display") require Matplotlib (>= 2.2.4). ### User installation If you already have a working installation of numpy and scipy, the easiest way to install FPTE is using `pip`: pip install -U FPTE or `install from source`: git clone https://github.com/MahdiDavari/FPTE cd FPTE python setup.py install In order to check your installation you can use: python -m pip show FPTE # to see which version and where FPTE is installed python -m pip freeze # to see all packages installed in the active virtualenv python -c "import FPTE; print(FPTE.__version__)" _Note that in order to avoid potential conflicts with other packages it is strongly recommended to use a virtual environment (venv)._ ## Theory **Elastic Stifness Coefficients from Stress-Strain Relations:** According to Hooke's law, the second-rank stress and strain tensors for a slightly deformed crystal are related by $$ $$ where the fourth rank tensors c<sub>ijkl</sub> and s<sub>ijkl</sub> are called the elastic stiffness coefficients and elastic compliance constants respectively. Here we deal with elastic stiffness coefficients c<sub>ijkl</sub>, which govern the proper stress-strain relations at nite strain. In general, we can write $$ $$ where X and x are the coordinates before and after the deformation. There are 81 independent stiffness coefficients in general; however, this number is reduced to 21 by the requirement of the complete Voigt symmetry. In Voigt notation (c<sub>ij</sub>), the elastic constants form a symmetric 6x6 matrix $$ $$ In single suffix notation (running from 1 to 6), we can also use the matrix representations for stress and strain $$ $$ <br> and $$ $$ where the stress components are &sigma;<sub>1</sub> = &sigma;<sub>xx</sub> ; &sigma;<sub>2</sub> = &sigma;<sub>yy</sub> ; &sigma;<sub>3</sub> = &sigma;<sub>zz</sub> ; &sigma;<sub>4</sub> = &sigma;<sub>yz</sub> ; &sigma;<sub>5</sub> = &sigma;<sub>zx</sub> ; &sigma;<sub>6</sub> = &sigma;<sub>xy</sub>, and the strain components are &epsilon;<sub>1</sub> = &epsilon;<sub> xx</sub> ; &epsilon;<sub>2</sub> = &epsilon;<sub>yy</sub> ; &epsilon;<sub>3</sub> = &epsilon;<sub>zz</sub> ; &epsilon;<sub>4</sub> = &epsilon;<sub>yz</sub> ; &epsilon;<sub>5</sub> = &epsilon;<sub>zx</sub> ; &epsilon;<sub>6</sub> = &epsilon;<sub>xy</sub>. When a crystal lattice is deformed with strain (&epsilon;), new lattice vectors a are related to old vectors ** a**<sub>0</sub> by **a** = (I + &epsilon;) **a**<sub>0</sub>, where I is identity matrix. The stress-strain relations are then simply given by $$ $$ The presence of the symmetry in the crystal reduces further the number of independent c<sub> ij</sub> . A cubic crystal having highest symmetry is characterized by the lowest number (only three) of independent elastic constants, c<sub>11</sub>, c<sub>12</sub> and c<sub>44</sub>, which in matrix notation is $$ $$ | Crystal System |Space Group Number |No. of Elastic Constants | |----------------|-------------------------------|-----------------------------| |`Cubic`|195-230 | 3 | |`Hexagonal` |168-194 |5 | |`Trigonal` |143-167|6-7| |`Tetragonal` |75-142 |6-7| |`Orthorhombic`| 16-74 | 9| |`Monoclinic` | 3-15| 13| |`Triclinic` | 1 and 2 | 21| > **Note:** For **more information** regarding the second-order elastic constant see reference: <br> 1. Golesorkhtabar, Rostam, et al., “ElaStic: A Tool for Calculating Second-Order Elastic Constants from First Principles.” Computer Physics Communications 184, no. 8 (2013): 1861–73. 2. Karki, Bijaya B. “High-Pressure Structure and Elasticity of the Major Silicate and Oxide Minerals of the Earth’s Lower Mantle,” 1997. 3. Barron, THK, and ML Klein. “Second-Order Elastic Constants of a Solid under Stress.” Proceedings of the Physical Society 85, no. 3 (1965): 523.


نیازمندی

مقدار نام
>=1.16.5 numpy
>=0.25.3 pandas
>=2.2.4 matplotlib
>=0.11 joblib
>=3.5.4 subprocess32
>=0.25.3 pandas
>=2.2.4 matplotlib
>=0.9.0 seaborn
>=0.57.0 memory-profiler
>=4.0.1 sphinx
>=0.7.0 sphinx-gallery
>=7.1.2 Pillow
>=1.3.0 sphinx-prompt
>=0.4.2 sphinxext-opengraph
>=0.25.3 pandas
>=2.2.4 matplotlib
>=0.9.0 seaborn
>=0.25.3 pandas
>=2.2.4 matplotlib
>=5.0.1 pytest
>=2.0.3 PyHamcrest
>=2.9.0 pytest-cov
>=4.0.0 pyamg


زبان مورد نیاز

مقدار نام
>=3.7 Python


نحوه نصب


نصب پکیج whl FPTE-1.2.1:

    pip install FPTE-1.2.1.whl


نصب پکیج tar.gz FPTE-1.2.1:

    pip install FPTE-1.2.1.tar.gz